PML-FDTD Analysis of Nonreciprocal Magnetic Photonic Crystals with Ferromagnetic Losses

Kyung‐Young Jung, B. Donderici, F. Teixeira
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引用次数: 2

Abstract

Nonreciprocal magnetic photonic crystals (MPCs) are dispersion engineered metamaterials that exhibit unique properties such as electromagnetic unidirectionality and frozen modes with zero group velocity [1], [2]. Nonreciprocal MPCs are periodic structures composed of misaligned anisotropic dielectric layers (A-layers) and ferromagnetic layers (F-layers), as shown in Fig. 1. MPCs with a proper choice of geometry and tensor parameters can display asymmetric dispersion relation ω(k) with a stationary inflection point (SIP) in a forward direction and no SIP in a backward direction [1]. Since group velocities are extremely low near the SIP, EM waves seem to be “frozen” inside nonreciprocal MPCs in the forward direction; at the same time, forward propagating EM pulses can exhibit a dramatic growth in amplitude inside the MPC. In the backward direction, EM waves inside the MPCs propagate in an ordinary fashion [2].
具有铁磁损耗的非互易磁性光子晶体的PML-FDTD分析
非互易磁光子晶体(MPCs)是一种色散工程超材料,具有独特的特性,如电磁单向性和零群速度的冻结模式[1],[2]。非互易MPCs是由各向异性介质层(a层)和铁磁层(f层)组成的周期性结构,如图1所示。适当选择几何和张量参数的MPCs可以显示不对称色散关系ω(k),其中正向有平稳拐点(SIP),而反向无SIP[1]。由于SIP附近的群速度极低,电磁波似乎被“冻结”在正向的非互反mpc内;同时,前向传播的电磁脉冲在MPC内的振幅会急剧增长。在反向方向上,电磁波在MPCs内以普通方式传播[2]。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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